Acceleration, Shock and Vibration Sensors

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Chapter 5 Piezoelectric Element Preload Ring Seismic Mass Accelerometer Base Figure 5.2.1: Basic piezoelectric accelerometer construction. The active elements of the accelerometer are the piezoelectric elements. The elements act as a spring, which has a stiffness k, and connect the base of the accelerometer to the seismic masses. When an input is present at the base of the accelerometer, a force (F) is created on piezoelectric material proportional to the applied acceleration (a) and size of the seismic mass (m). (The sensor is governed by Newton’s law of motion F = ma.) The force experienced by the piezoelectric crystal is proportional to the seismic mass times the input acceleration. The more mass or acceleration, the higher the applied force and the more electrical output from the crystal. The frequency response of the sensor is determined by the resonant frequency of the sensor, which can generally be modeled as a simple single degree of freedom system. Using this system, the resonant frequency (ω) of the sensor can be estimated by: ω = k / m . The typical frequency response of piezoelectric accelerometers is depicted in Figure 5.2.2. Piezoelectric accelerometers can be broken down into two main categories that define their mode of operation. Internally amplified accelerometers or IEPE (internal Relative Amplitude Resonance Peak electronic piezoelectric) con- Vibration of tain built-in microelectronic Seismic Mass signal conditioning. Charge mode accelerometers con- Useful Frequency Range tain only the self-generating piezoelectric sensing element and have a high impedance Vibration of Base charge output signal. Relative Frequency Figure 5.2.2 Typical frequency response of piezoelectric accelerometer. 138
Acceleration, Shock and Vibration Sensors IEPE Accelerometers IEPE sensors incorporate built-in, signal-conditioning electronics that function to convert the high-impedance charge signal generated by the piezoelectric sensing element into a usable low-impedance voltage signal that can be readily transmitted, over ordinary two-wire or coaxial cables, to any voltage readout or recording device. The low-impedance signal can be transmitted over long cable distances and used in dirty field or factory environments with little degradation. In addition to providing crucial impedance conversion, IEPE sensor circuitry can also include other signal conditioning features, such as gain, filtering and self-test features. The simplicity of use, high accuracy, broad frequency range, and low cost of IEPE accelerometer systems make them the recommended type for use in most vibration or shock applications. However, an exception to this assertion must be made for circumstances in which the temperature at the installation point exceeds the capability of the built-in circuitry. The routine upper temperature limit of IEPE accelerometers is 250°F (121°C); however, specialty units are available that operate to 350°F (175°C). IEPE is a generic industry term for sensors with built-in electronics. Many accelerometer manufacturers use their own registered trademarks or trade name to signify sensors with built-in electronics. Examples of these names include: ICP® (PCB Piezotronics), Deltatron (Bruel & Kjaer), Piezotron (Kistler Instruments), and Isotron (Endevco), to name a few. The electronics within IEPE accelerometers require excitation power from a constantcurrent, DC voltage source. This power source is sometimes built into vibration meters, FFT analyzers and vibration data collectors. A separate signal conditioner is required when none is built into the readout. In addition to providing the required excitation, power supplies may also incor- Figure 5.2.3: Typical IEPE system. porate additional signal conditioning, such as gain, filtering, buffering and overload indication. The typical system set-ups for IEPE accelerometers are shown in Figure 5.2.3. 139
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Acceleration, Shock and Vibration Sensors

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